While the first law of thermodynamics focuses on the conservation of energy, it doesn't address the direction in which processes occur. [1]
The second law of thermodynamics complements the first law by:
Establishing the direction of processes, indicating that they proceed in a specific direction, not spontaneously in reverse. [2]
Recognising that energy possesses quality in addition to quantity. [3]
A process must adhere to both the first and second laws of thermodynamics to occur. [2]
Thermal Energy Reservoirs: Hypothetical bodies with large thermal energy capacity that can exchange heat without changing temperature. Examples include oceans, lakes, and the atmosphere. [4, 5]
Heat Engines: Devices that operate in a cycle, receiving heat from a high-temperature source, converting some to work, and rejecting waste heat to a low-temperature sink. [6]
Thermal Efficiency: The ratio of net work output to total heat input, measuring a heat engine's effectiveness. [7]
Refrigerators: Cyclic devices that transfer heat from a low-temperature space to a high-temperature environment, requiring work input. [8, 9]
Coefficient of Performance (COPR): Indicates a refrigerator's efficiency, defined as the ratio of heat removed from the cooled space to the required work input. [10]
Heat Pumps: Similar to refrigerators, heat pumps transfer heat from a low-temperature source to a high-temperature space, but their objective is heating. [11]
Coefficient of Performance (COPHP): Measures a heat pump's efficiency, defined as the ratio of heat supplied to the heated space to the required work input. [12]
Kelvin-Planck Statement: It's impossible for a cyclic device to receive heat from a single reservoir and produce net work. In other words, a heat engine must reject some heat to a low-temperature sink for continuous operation. [13]
Clausius Statement: It's impossible to construct a device that operates in a cycle, producing no effect other than transferring heat from a lower-temperature body to a higher-temperature body. In other words, external work input is needed to transfer heat from cold to hot. [14]
Both the Kelvin-Planck and Clausius statements are negative and equivalent expressions of the second law. [15]
Perpetual-motion machines are hypothetical devices that violate either the first or second law of thermodynamics. [16]
Perpetual-motion machine of the first kind (PMM1): Violates the first law by creating energy. [16]
Perpetual-motion machine of the second kind (PMM2): Violates the second law. For example, a heat engine claiming 100% efficiency. [16, 17]
Reversible processes are idealised processes that can be reversed without leaving any trace on the surroundings. [18]
They are theoretical limits for corresponding irreversible processes, which occur in reality. [19]
Irreversibilities are factors that cause a process to be irreversible. Examples include: [20]
Friction [21]
Unrestrained expansion [21]
Heat transfer across a finite temperature difference [22]
Mixing of fluids [20]
Electric resistance [20]
Inelastic deformation [20]
Chemical reactions [20]
Minimising irreversibilities in engineering systems maximises efficiency. [19]
A process is internally reversible if no irreversibilities occur within the system boundaries. [23]
A process is externally reversible if no irreversibilities occur outside the system boundaries. [23]
A process is totally reversible (simply reversible) if it involves no irreversibilities within the system or its surroundings. [24]
The Carnot cycle is a theoretical cycle consisting of four reversible processes: [25-27]
Reversible Isothermal Expansion
Reversible Adiabatic Expansion
Reversible Isothermal Compression
Reversible Adiabatic Compression
The Carnot cycle is the most efficient cycle operating between two specific temperature limits. [28]
Reversed Carnot Cycle: The Carnot cycle can be reversed to represent a refrigeration cycle, where the direction of heat and work interactions are flipped. [28]
Efficiency Comparison: The efficiency of an irreversible heat engine is always less than the efficiency of a reversible heat engine operating between the same two reservoirs. [29, 30]
Efficiency Equality: The efficiencies of all reversible heat engines operating between the same two reservoirs are the same. [29, 31]
A thermodynamic temperature scale is independent of the properties of substances used to measure temperature. [32]
The Kelvin scale is a thermodynamic temperature scale where the ratio of absolute temperatures is defined based on the ratio of heat transfers between a reversible heat engine and the reservoirs. [33]
Absolute Zero: The theoretical lower limit of temperature, 0 K or -273.15°C, where molecular motion ceases. [33]
Triple Point of Water: The state where all three phases of water exist in equilibrium, assigned the value of 273.16 K. [34]
The Carnot heat engine is a hypothetical engine operating on the reversible Carnot cycle. [35]
Its efficiency is the maximum possible for any heat engine operating between the same temperature limits: [35]
ηth,rev = 1 - TL/TH
where TL and TH are the absolute temperatures of the low- and high-temperature reservoirs, respectively.
The efficiency of a Carnot heat engine increases with increasing TH and decreases with increasing TL. [36]
Carnot refrigerator and Carnot heat pump are hypothetical devices operating on the reversed Carnot cycle. [37]
Their COPs are the maximum possible for any refrigerator or heat pump operating between the same temperature limits: [37]
COPR,rev = TL / (TH - TL)
COPHP,rev = TH / (TH - TL)
The COPs of actual refrigerators and heat pumps are always lower than the corresponding Carnot COPs. [38]
Higher-temperature thermal energy can be converted to work more efficiently, indicating a higher quality of energy. [39]
The sources only mention the quality of energy in relation to its temperature. Information regarding other factors affecting energy quality would need to be independently verified.